<p>Glass samples of CuO/Fe<sub>2</sub>O<sub>3</sub> reinforced bismuth borate containing ZnO and NaF with the chemical form 65B<sub>2</sub>O<sub>3</sub>-15NaF-15ZnO- 5Bi<sub>2</sub>O<sub>3</sub>-XFe<sub>2</sub>O<sub>3</sub>- YCuO: (X,Y) = (0.0,0.0) {S0}, (0.1, 0.4) {S1}, (0.2, 0.3) {S2}, (0.3, 0.2) {S3}, (0.4, 0.1) {S4}, and (0.5, 0.0) {S5} mol.% were prepared via melt quenching procedure. The influence of CuO/Fe<sub>2</sub>O<sub>3</sub> on the structure, physical properties, and <i>γ</i>-ray attenuation capability was examined. The non-crystallinity nature of samples was confirmed by XRD measurements and SEM images. The density (D<sub>s</sub>) of samples increased from 3.10 to 3.30&#xa0;g/cm<sup>3</sup> as Fe<sub>2</sub>O<sub>3</sub>concentration increase from 0.0 to 0.5&#xa0;mol.%. The molar volume (V<sub>m</sub>) declined from 28.05 to 26.62&#xa0;cm<sup>3</sup>/mol. The parameter of oxygen packing density (OPD) enhanced from 80.20 to 85.09. The oxygen molar volume (OMV) changed as 12.47&#xa0;cm<sup>3</sup>/mol for S0 sample and 11.75&#xa0;cm<sup>3</sup>/mol for S5 sample. Direct (E<sub>opt-direct</sub>) and indirect (E<sub>opt-indirect</sub>) optical band gaps decreased with doping with Fe<sup>+3</sup> and Cu<sup>2+</sup> ions in the glass networks. E<sub>opt-direct</sub> decreased from 3.685 to 3.620&#xa0;eV, while E<sub>opt-indirect</sub> varied between 3.642 and 3.595&#xa0;eV. Undoped sample S0 exhibited a broad strong UV absorption which related to unavoidable trace ferric ions, Fe<sup>3+</sup> ions, impurities contaminated within the raw materials used for the preparation of the glasses. For doped glasses UV-visible bands due to doping with 3d transition metal ions. In terms of <i>γ</i>-ray shielding, linear (LAC) absorption coefficient followed the order: S0<sub>LAC</sub> &lt; S1<sub>LAC</sub> &lt; S2<sub>LAC</sub> &lt; S3<sub>LAC</sub> &lt; S4<sub>LAC</sub> &lt; S5<sub>LAC</sub>. The S5 glass sample has the lowest half value layer (HVL) and mean free path (MFP). The effective atomic number (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({\text{Z}}_{\text{eff}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Z</mtext> <mtext>eff</mtext> </msub> <mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> has the same trend of MAC. The suggested S5 sample presents the best <i>γ</i>-ray shielding capability among the investigated samples. Results confirm that the sample coded as S5 is superior as <i>γ</i>-ray shields compared to ordinary concrete (OC) and RS-253-G18 glasses.</p>

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Structural, Physical, Optical Properties as well γ-ray Attenuation Capability of Bismuth Borate Containing Fe2O3 and CuO: Potential Use in Optical and Radiation Shielding Applications

  • Nada Alfryyan,
  • Norah A. M. Alsaif,
  • Hanan Al-Ghamdi,
  • Shaaban M. Shaaban,
  • M. S. Shams,
  • Adel M. El-Refaey,
  • R. A. Elsad,
  • A. M. Abdelghany,
  • Y. S. Rammah

摘要

Glass samples of CuO/Fe2O3 reinforced bismuth borate containing ZnO and NaF with the chemical form 65B2O3-15NaF-15ZnO- 5Bi2O3-XFe2O3- YCuO: (X,Y) = (0.0,0.0) {S0}, (0.1, 0.4) {S1}, (0.2, 0.3) {S2}, (0.3, 0.2) {S3}, (0.4, 0.1) {S4}, and (0.5, 0.0) {S5} mol.% were prepared via melt quenching procedure. The influence of CuO/Fe2O3 on the structure, physical properties, and γ-ray attenuation capability was examined. The non-crystallinity nature of samples was confirmed by XRD measurements and SEM images. The density (Ds) of samples increased from 3.10 to 3.30 g/cm3 as Fe2O3concentration increase from 0.0 to 0.5 mol.%. The molar volume (Vm) declined from 28.05 to 26.62 cm3/mol. The parameter of oxygen packing density (OPD) enhanced from 80.20 to 85.09. The oxygen molar volume (OMV) changed as 12.47 cm3/mol for S0 sample and 11.75 cm3/mol for S5 sample. Direct (Eopt-direct) and indirect (Eopt-indirect) optical band gaps decreased with doping with Fe+3 and Cu2+ ions in the glass networks. Eopt-direct decreased from 3.685 to 3.620 eV, while Eopt-indirect varied between 3.642 and 3.595 eV. Undoped sample S0 exhibited a broad strong UV absorption which related to unavoidable trace ferric ions, Fe3+ ions, impurities contaminated within the raw materials used for the preparation of the glasses. For doped glasses UV-visible bands due to doping with 3d transition metal ions. In terms of γ-ray shielding, linear (LAC) absorption coefficient followed the order: S0LAC < S1LAC < S2LAC < S3LAC < S4LAC < S5LAC. The S5 glass sample has the lowest half value layer (HVL) and mean free path (MFP). The effective atomic number ( \({\text{Z}}_{\text{eff}})\) Z eff ) has the same trend of MAC. The suggested S5 sample presents the best γ-ray shielding capability among the investigated samples. Results confirm that the sample coded as S5 is superior as γ-ray shields compared to ordinary concrete (OC) and RS-253-G18 glasses.